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Description Enables a page author to declaratively register an ActionListener instance on a UIComponent Enables a page author to declaratively add Ajax behavior to the UIComponent associated with the parent tag, or adds Ajax behavior to the UIComponent(s) associated with any child tags Enables a page author to declaratively set an attribute value on a UIComponent Enables a page author to declaratively register a DateTimeConverter instance on a UIComponent

If the tube is only partially filled with liquid (the remainder being vapor in equilibrium with the liquid), heating at first causes changes described by the vapor-pressure curve (solid line) of Fig 33 For the process indicated by line J Q on Fig 32(b), the meniscus is initially near the top of the tube (point J), and the liquid expands upon heating until it completely fills the tube (point Q) On Fig 33 the process traces a path from (J, K ) to Q, and with further heating departs from the vapor-pressure curve along the line of constant molar volume v, The process indicated by line K N on Fig 32(b) starts with a lower meniscus level in the tube (point K); heating causes liquid to vaporize, and the meniscus recedes to the bottom of the tube (point N) On Fig 33 the process traces a path from ( J , K) to N With further heating the path continues along the line of constant molar volume V For a unique filling of the tube, with a particular intermediate meniscus level, the heating process follows a vertical line on Fig 32(b) that passes through the critical point C Physically, heating does not produce much change in the level of the meniscus As the critical point is approached, the meniscus becomes indistinct, then hazy, and finally disappears On Fig 33 the path first follows the vapor-pressure curve, proceeding from point ( J , K) to the critical point C, where it enters the single-phase fluid region, and follows V,, the line of constant molar volume equal to the critical volume of the fluid

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JSF Version(s) 10, 11, 12, 20 20

int ch; while ((ch = inputstreamread()) != -1) { bytestreamwrite(ch); } str = new String(bytestreamtoByteArray()); bytestreamclose(); } Systemoutprintln(str); } } catch(IOException error) { Systemoutprintln("Caught IOException: " + errortoString()); } finally { if (inputstream!= null) { try { inputstreamclose(); } catch( Exception error) { /*log error*/ } } if (connection != null) { try { connectionclose(); } catch( Exception error) { /*log error*/ } } } } } }

For the regions of the diagram where a single phase exists, Fig 32(b) implies a relation connecting P, V, and T which may be expressed by the functional equation:

10, 11, 12, 20 10, 11, 12, 20

Listing 13-8 The JAD file for Listing 13-7

TABLE 16-1

This means that an equation o state exists relating pressure, molar or specific volume, and f temperature for any pure homogeneous fluid in equilibrium states The simplest equation of state is for an ideal gas, P V = RT, a relation which has approximate validity for the lowpressure gas region of Fig 32(b), and which is discussed in detail in Sec 33 An equation of state may be solved for any one of the three quantities P , V, or T as a function of the other two For example, if V is considered a function of T and P , then V = V(T, P), and

The Standard Core Library Quick Reference (continued)

13:

The partial derivatives in this equation have definite physical meanings, and are related to two properties, commonly tabulated for liquids, and defined as follows:

Part III:

MIDlet-Jar-URL: httpconnectionjar MIDlet-1: httpconnection, , httpconnection MicroEdition-Configuration: CLDC-10 MicroEdition-Profile: MIDP-10 MIDlet-JAR-SIZE: 100

Volume expansivity:

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